Physics 111 Homework Solutions Week #9 - Thursday

Similar documents
Physics 111 Homework Solutions Week #9 - Friday

λ φ φ = hc λ ev stop φ = λ φ and now ev stop λ ' = Physics 220 Homework #2 Spring 2016 Due Monday 4/11/16

1.4 The Compton Effect

Mechanics and Special Relativity (MAPH10030) Assignment 4

EE 4395 Special Topics Applied Quantum Mechanics for Electrical Engineers Homework Problems

Recitation on the Compton effect Solution

1 (a) Sketch the electric field surrounding the gold nucleus drawn below. (3)

[1+ m2 c 4 4EE γ. The equations of conservation of energy and momentum are. E + E γ p p γ

Welcome back to PHY 3305

Welcome back to PHY 3305

Chapter 22 Quantum Mechanics & Atomic Structure 22.1 Photon Theory of Light and The Photoelectric Effect Homework # 170

Chapter 10: Wave Properties of Particles

Physics 202H - Introductory Quantum Physics I Midterm Test - A - Solutions

Exercise 1 Atomic line spectra 1/9

Chapter 27 Early Quantum Theory and Models of the Atom Discovery and Properties of the electron

Physics 102: Lecture 23

Chapters 28 and 29: Quantum Physics and Atoms Questions & Problems

Lecture 15 Notes: 07 / 26. The photoelectric effect and the particle nature of light

PARTICLES AND WAVES CHAPTER 29 CONCEPTUAL QUESTIONS

Physics 202. Professor P. Q. Hung. 311B, Physics Building. Physics 202 p. 1/2

Particles and Waves Particles Waves

Welcome back to PHY 3305

1240 ev nm nm. f < f 0 (5)

Exam Review Practice Questions. Electric Forces. the force is zero. Four charges are fixed at the corners of a square of sides 4 m as shown.

Marian Physics! Planck to Bohr. Flat Prairie Publishing

Physics 102: Lecture 23

Final Exam Sample Problems

General Physics (PHY 2140) Lecture 15

Lecture 3 - Compton Scattering

PHYS 3313 Section 001 Lecture #7

Massachusetts Institute of Technology

Physics Modern Physics Professor Jodi Cooley. Welcome back. to PHY Arthur Compton

Rb, which had been compressed to a density of 1013

DUAL NATURE OF RADIATION AND MATTER

Physics 111 Homework Solutions Week #10 - Thursday

Ch., Problem 3 After acceleration through 0 MV both the electron and proton will each have a kinetic energy of 0 MeV. For the electron, E K + mc 0:5 M

Physics 1C Lecture 28C. "For those who are not shocked when they first come across quantum theory cannot possibly have understood it.

13.2 NUCLEAR PHYSICS HW/Study Packet

Announcements. Lecture 8 Chapter. 3 Wave & Particles I. EM- Waves behaving like Particles. The Compton effect (Arthur Compton 1927) Hypothesis:

PHYS120 Lecture 5 - Energy, momentum and mass 5-1

The wavefunction ψ for an electron confined to move within a box of linear size L = m, is a standing wave as shown.

CHAPTER 12 TEST REVIEW

Chapter 30 Quantum Physics 30.1 Blackbody Radiation and Planck s Hypothesis of Quantum Energy 30.2 Photons and the Photoelectric Effect 30.

The Bohr Model of Hydrogen

λ = h = h p mv λ = h mv FXA 2008 Candidates should be able to :

Circlon Coil Spin of Electrons & Protons. 4 Photon Energies. Rotational Kinetic Energy. Linear Kinetic Energy. Negative Electric Coils.

MITOCW watch?v=wr88_vzfcx4

PSI AP Physics How was it determined that cathode rays possessed a negative charge?

Chapter 4: The Wave Nature of Matter

State the main interaction when an alpha particle is scattered by a gold nucleus

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS IB PHYSICS

Anti Compton effect (1). A.M.shehada. Division of physics, Sciences college, Damascus university, Syria

We start with a reminder of a few basic concepts in probability. Let x be a discrete random variable with some probability function p(x).

Chapter NP-4. Nuclear Physics. Particle Behavior/ Gamma Interactions TABLE OF CONTENTS INTRODUCTION OBJECTIVES 1.0 IONIZATION

Chapter 27 Quantum Physics

Radiation Physics PHYS /251. Prof. Gocha Khelashvili

PHYS 3313 Section 001 Lecture #11

3A. Average specific heat of each free electron at constant volume

Which of the following can be used to calculate the resistive force acting on the brick? D (Total for Question = 1 mark)

Dual Nature of Radiation and Matter GLIMPSES 1. Electron. It is an elementary particle having a negative charge of 1.6x C and mass 9.1x kg

Chapter 2 Problem Solutions

Quantum Physics Lecture 3

Chapter 37 Early Quantum Theory and Models of the Atom. Copyright 2009 Pearson Education, Inc.

Welcome back to PHY 3305

Outline. Chapter 6 The Basic Interactions between Photons and Charged Particles with Matter. Photon interactions. Photoelectric effect

English CPH E-Book Theory of CPH Section 2 Experimental Foundation of CPH Theory Hossein Javadi

Announcements. Lecture 8 Chapter. 3 Wave & Particles I. Albert Einstein proposed: The Photoelectric Effect (Albert Einstein 1905)

Slide 1 / 57. Nuclear Physics & Nuclear Reactions Practice Problems

REDEFINING IONISATION ENERGY OF AN H-ATOM PART 1. Elementary charge associated with a photon x C

Applied Nuclear Physics (Fall 2006) Lecture 19 (11/22/06) Gamma Interactions: Compton Scattering

ESSENTIAL QUANTUM PHYSICS PETER LANDSHOFF. University of Cambridge ALLEN METHERELL. University of Central Florida GARETH REES. University of Cambridge

Unit 6 Modern Physics

PHYSICS 3204 PUBLIC EXAM QUESTIONS (Quantum pt.1)

Lecture 22 Ion Beam Techniques

normalized spectral amplitude R(λ)

Department of Natural Sciences Clayton State University. Physics 3650 Quiz 1

Physics 100 PIXE F06

Photoelectric effect

Chapter 2. Relativity 2

Interaction of Ionizing Radiation with Matter

AP Physics Study Guide Modern Physics I. Atomic Physics and Quantum Effects 1. Who is generally credited with the discovery of the electron?

Fall 2012 Qualifying Exam. Part I

Shell Atomic Model and Energy Levels

Quantum Theory of Light

A fluorescent tube is filled with mercury vapour at low pressure. After mercury atoms have been excited they emit photons.

University of California, Berkeley Physics H7C Spring 2011 (Yury Kolomensky) THE FINAL EXAM Monday, May 9, 7 10pm. Maximum score: 200 points

Kinetic Energy: K = (γ - 1)mc 2 Rest Energy (includes internal kinetic and potential energy): E R mc 2

Physics 3204 UNIT 3 Test Matter Energy Interface

tip conducting surface

Physics 121 Hour Exam #5 60 Minutes, Take Home, Closed Book

Explain how Planck resolved the ultraviolet catastrophe in blackbody radiation. Calculate energy of quanta using Planck s equation.

Lecture 14 (11/1/06) Charged-Particle Interactions: Stopping Power, Collisions and Ionization

Lecture 2: Quantum Mechanics and Relativity

1 The Cathode Rays experiment is associated. with: Millikan A B. Thomson. Townsend. Plank Compton

Possible Interactions. Possible Interactions. X-ray Interaction (Part I) Possible Interactions. Possible Interactions. section

5.111 Principles of Chemical Science

Chapter 38. Photons and Matter Waves

Physics 1C. End of Chapter 30 Exam Preparationds

Lecture Outline Chapter 30. Physics, 4 th Edition James S. Walker. Copyright 2010 Pearson Education, Inc.

SPH4U UNIVERSITY PHYSICS

Transcription:

Physics 111 Homework Solutions Week #9 - Thursday Monday, March 1, 2010 Chapter 24 241 Based on special relativity we know that as a particle with mass travels near the speed of light its mass increases In order to accelerate this object from rest to a speed near that of light would require an ever increasing force (one that rapidly becomes larger by a factor of γ) There are no known forces that could accelerate a particle with mass to the speed of light in a finite amount of time with a finite amount of energy So for objects with no rest mass, as they travel at the speed of light, there mass does not increase with increasing speed we avoid these problems of accelerating the massless particles 246 The Compton shift in wavelength for the proton the electron are given by Δλ e = h 1 cosφ m e c ( ) Δλ p = h ( 1 cosφ)respectively Evaluating the ratio c of the shift in wavelength for the proton to the electron, evaluated at the same detection angle φ, we find Δλ p = hm c e Δλ e ch = m e = 5 10 4 Δλ p = 5 10 4 Δλ e Therefore the shift in wavelength for the proton is smaller than the wavelength shift for the electron Multiple-Choice Problems Relativistic energy momentum for an object of mass m For an object with a m = 1kg rest mass, it has a rest energy of E = mc 2 = 9x10 16 J The Lorentz factor is given by:, with the relativistic momentu = γmv, the relativistic energy E 2 = p 2 c 2 +m 2 c 4 a For a velocity of 08c, The relativistic momentum energy are therefore,

b Following the procedure in part a, for a velocity of 09c,, the relativistic momentum is 619x10 8 kgm/s, the relativistic energy is 207x10 17 J c For a velocity of 095c, γ = 320, the relativistic momentum is 913x10 8 kgm/s, the relativistic energy is 288x10 17 J d For a velocity of 099c, γ = 709, the relativistic momentum is 211x10 9 kgm/s, the relativistic energy is 6387x10 17 J e For a velocity of 0999c, γ = 224, the relativistic momentum is 670x10 9 kgm/s, the relativistic energy is 20x10 18 J 242 For an electron with rest mass 911x10-31 kg, it has a rest energy of E = mc 2 = 8199x10-14 J = 0511 MeV The Lorentz factor is given by:, the relativistic momentum energy are given respectively as p = γmv a For the electron with a velocity of 08c, γ = 167 The relativistic momentum energy are therefore, Using the fact that 16x10-19 J = 1 ev, the relativistic energy is given as Further it can be shown that the total relativistic energy is given as Thus the relativistic energy can be computed in a more efficient method b Following the method outlined in part a, for a velocity of 09c, γ = 229 The relativistic momentum is therefore, c For a velocity of 095c, γ = 32 The relativistic momentum is therefore, d For a velocity of 099c, γ = 709 The relativistic momentum is therefore, e For a velocity of 0999c, γ = 224 The relativistic momentum is therefore,

From equation (2) we have the kinetic energy given by Using the fact that v << c, we can use the binomial expansion on the Lorentz factor for small arguments This gives Therefore the equation for the kinetic energy becomes which is the classical expression for kinetic energy 244 Will be posted once all of the homework has been turned in 247 For a photon, a its momentum is given by b its wavelength is given by the de Broglie relation c its frequency is given by 2413 The relativistic energy is given as The rest energy, mc 2 is 8199x10-19 J = 0511 MeV From the de Broglie wavelength we can calculate the momentum of the electron, Thus the relativistic energy is Wednesday, March 3, 2010 Chapter 24 Multiple-Choice

Problems 2411 A Compton Effect experiment a The wavelength momentum of the incident gamma ray are given as respectively b Using the Compton formula for the wavelength of the scattered photon the fact that the energy is inversely proportional to the wavelength we can write c The energy of the scattered gamma ray photon is mass of the electron is given as where the rest d The kinetic energy of the recoiling electron is found using conservation of energy where when the incident gamma ray photon interacts with electrons in the sample, the gamma ray photon loses some energy to the electron as it scatters Thus the kinetic energy of the recoiling electron is e The speed of the recoiling electron is given by using the expression for the relativistic kinetic energy We have 2412 X-rays on a foil target a The energy is given by b The scattered wavelength is given by

Thus, The energy is given by the formula in part a, is 118x10-14 J = 00741 MeV c The energy given to the foil is